Switchable interleaved channel separator devices and systems

ABSTRACT

The present invention provides an improved switchable interleaved channel separator device. The switchable interleaved channel separator device utilizes an adjustable reflective non-linear interferometer, which performs both switching and wavelength polarization sorting functions, so that overall complexity of the device is reduced. Further, because the adjustable non-linear interferometer is a reflection element, signal light paths are folded back upon one another so as to realize an overall reduction in the device&#39;s size, as well as the capability of performing optical couplings predominantly or wholly at a single side or at adjacent sides of the device.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a DIVISIONAL application of U.S. patent application Ser. No. 09/772,684, entitled “Switchable Interleaved Channel Separator Devices and Systems,” filed on Jan. 30, 2001 now U.S. Pat. No. 6,614,573.

FIELD OF THE INVENTION

The present invention relates to optical networks, and more particularly, to optical switching, routing, multiplexing and de-multiplexing devices.

BACKGROUND OF THE INVENTION

The use of optical fiber for long-distance transmission of voice and/or data is now common. As the demand for data carrying capacity continues to increase, there is a continuing need to utilize the bandwidth of existing fiber-optic cable more efficiently. An established method for increasing the carrying capacity of existing fiber cable is Wavelength Division Multiplexing (WDM) in which multiple information channels are independently transmitted over the same fiber using multiple wavelengths of light. In this practice, each light-wave-propagated information channel corresponds to light within a specific wavelength range or “band.”

In this document, these individual information-carrying lights are referred to as either “signals” or “channels.” The totality of multiple combined signals in a wavelength-division multiplexed optical fiber, optical line or optical system, wherein each signal is of a different wavelength range, is herein referred to as a “composite optical signal.”

Because of the increased network traffic resulting from the use of the WDM technique, there is an increasing need for sophisticated optical switching and routing devices which can quickly route or re-route numerous channels amongst various optical communications lines. FIG. 14 illustrates a known apparatus that performs this function. This apparatus 300 has two control states and serves to separate channels of the wavelength spectrum applied to an input port 11 and determines which of two output ports 13, 14 are coupled to each of the channels. The input WDM signal enters the first birefringent element 30 that spatially separates horizontal and vertically polarized components of the WDM signal. The first birefringent element 30 allows the vertically polarized portion of the optical signal to pass through without changing course. In contrast, horizontally polarized waves are redirected at an angle because of the birefringent walk-off effect. The horizontally polarized component travels along a path 301 as an extraordinary signal in the first birefringent element 30 while the vertically polarized component 302 travels as an ordinary signal and passes through without spatial reorientation.

Both the horizontally and vertically polarized components 301 and 302 are coupled to a switchable polarization rotator 40 under control of a control bit. The polarization rotator 40 consists of two sub-element rotators that form a complementary state, i.e. when one turns on the other turns off, such that, in general, the rotator 40 rotates the signals by either 0° (i.e., no rotation) or 90°. FIG. 14 illustrates one control state in which the signal 302 is rotated by 90° so that both signals 303, 304 exiting the rotator 40 have a horizontal polarization.

The stacked waveplates element 61 is a stacked plurality of birefringent waveplates at selected orientations that generate two eigen states. The first eigen state carries a first sub-spectrum with the same polarization as the input, and the second eigen state carries a complementary sub-spectrum at the orthogonal polarization. With horizontal polarizations 303, 304 input to the stacked waveplates clement 61 as shown in FIG. 14, orthogonal vertical and horizontal polarizations are generated with the first spectral band residing in horizontal polarization and the second spectral band residing in vertical polarization. With vertical polarizations 303, 304 input to the stacked waveplates element 61 orthogonal vertical and horizontal polarizations are generated with the first spectral band residing in vertical polarization and the second spectral band residing in horizontal polarization.

The pairs of optical responses 305, 306 output by the stacked waveplates element 61 are coupled to a second birefringent element 50. This birefringent element 50 has a similar construction to the first birefringent element 30 and spatially separates the horizontally and vertically polarized components of the input optical signals 305 and 306. As shown in FIG. 14, the optical signals 305, 306 are broken into vertically polarized components 307, 308 containing the second spectral band and horizontally polarized components 309, 310 containing the first spectral band. Due to the birefringent walk-off effect, the two orthogonal polarizations that carry first spectral band 309, 310 in horizontal polarization and second set spectral band 307, 308 in vertical polarization are separated by the second birefringent element 50.

Following the second birefringent element 50, the optical elements on the input side of the second birefringent element 50 can be repeated in opposite order, as illustrated in FIG. 14. The second stacked waveplates element 62 has substantially the same composition as the first stacked waveplates element 61. The horizontally polarized beams 309, 310 input to the second stacked waveplates element 62, are further purified and maintain their polarization when they exit the second stacked waveplates element 62. On the other hand, the vertically polarized beams 307, 308 experience a 90° polarization rotation and are also purified when they exit the second stacked waveplates element 62. The 90° polarization rotation is due to the fact that the vertically polarized beams 307, 308 carry the second spectral band and therefore are in the complementary state of element 62. At the output of the stacked waveplates element 62, all four beams 311, 312 and 313, 314 have horizontal polarization.

To recombine the spectra of the two sets of beams 311, 312 and 313, 314, a second polarization rotator 41 and a second birefringent element 70 are used. The second rotator 41 has two sub-elements that intercept the four parallel beams 311-314. The two sub-elements of the second rotator 41 are set at a complementary state to the first rotator 40. In the state illustrated in FIG. 14, the polarization of beams 311 and 313 is rotated by 90°, and beams 312 and 314 are passed without change of polarization. This results in an orthogonal polarization pair 315, 316 and 317, 318 for each spectral band at the output of the second rotator 41. Finally, a second birefringent element 70 re-combines the two orthogonal polarizations 315, 316 and 317, 318 using the walk-off effect to produce two spectra that exit at ports 14 and 13, respectively. In the operational state shown in FIG. 14, the first and second spectral bands exit at ports 13 and 14, respectively. In the other operational state of the apparatus 300, the outputs of the two spectral bands are reversed.

Although the known apparatus 300 (FIG. 14) appears to be capable of performing its intended function, the structure of the apparatus 300 entails undesirable complexity since separate sets of elements perform the functions of switching the operational state of the apparatus 300 and of sorting the polarizations of channels according to their respective wavelengths. In the apparatus 300, the polarization rotators 40-41 and the wavelength filters 61-62, respectively, perform the switching and sorting operations. Further, since all the various functions of the apparatus 300 are performed by transmissive optical elements, the input port 11 and output ports 13-14 must necessarily be disposed at opposite sides of the apparatus 300. Such a disposition causes the apparatus 300 to be excessively large and creates difficulty for coupling the apparatus 300 to fiber ferrules or ribbon cables in which all the fibers are disposed within a single bundle or group.

Accordingly, there exists a need for an improved switchable interleaved channel separator. The improved switchable interleaved channel separator should perform the functions of switching and wavelength polarization sorting within a single element to reduce size and complexity of the apparatus. These functions should be performed by a reflection element so as to facilitate external optical coupling to the apparatus predominantly at a single side or at adjacent sides of the separator. The present invention addresses such a need.

SUMMARY OF THE INVENTION

The present invention provides an improved switchable interleaved channel separator device. The switchable interleaved channel separator device utilizes an adjustable reflective non-linear interferometer, which performs both switching and wavelength polarization sorting functions, so that overall complexity of the device is reduced. Further, because the adjustable non-linear interferometer is a reflection element, signal light paths are folded back upon one another so as to realize an overall reduction in the device's size, as well as the capability of performing optical couplings predominantly or wholly at a single side or at adjacent sides of the device.

BRIEF DESCRIPTION OF THE FIGURES

FIG. 1a is a functional signal routing diagram of a switchable interleaved channel separator device in accordance with the present invention, as a 2×2 device.

FIG. 1b is a functional signal routing diagram of the switchable interleaved channel separator device in accordance with the present invention, as a 1×2 device.

FIG. 2 is a side view of a first preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention.

FIG. 3 is a side view of a second preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention.

FIG. 4 is an end view of the fiber configuration of the input and output fibers utilized within the second preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention.

FIG. 5a is a sequence of cross sectional views through the switchable interleaved channel separator device of FIG. 3 illustrating the locations and polarization states of fiber images created by the light of signals and sub-signals of a first set of wavelength division multiplexed channels.

FIG. 5b is a sequence of cross sectional views through the switchable interleaved channel separator device of FIG. 3 illustrating the locations and polarization states of fiber images created by the light of signals and sub-signals of a second set of wavelength division multiplexed channels.

FIGS. 6a-6 c each is a top view and a side view of a third preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention.

FIG. 6d is a view of a polarizing input/output port assembly utilized within the third preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention.

FIGS. 7a-7 b are side views of a fourth preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention.

FIGS. 8a-8 c are each a top view and a side view of a fifth preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention.

FIGS. 9a-9 c are illustrations of three preferred embodiments of an adjustable non-linear interferometer that may be utilized in the switchable interleaved channel separator device in accordance with the present invention.

FIG. 9d is a pair of schematic graphs of the spectrum of the polarization-rotated light and the spectrum of the polarization-non-rotated light reflected from an adjustable non-linear interferometer in two different operational states.

FIG. 10 is an illustration of a first preferred embodiment of an optical communications system that utilizes the switchable interleaved channel separator device in accordance with the present invention.

FIG. 11 is an illustration of a second preferred embodiment of an optical communications system that utilizes the switchable interleaved channel separator device in accordance with the present invention.

FIGS. 12a-12 c are illustrations of a programmable optical add/drop multiplexer that utilizes the switchable interleaved channel separator device in accordance with the present invention.

FIG. 13 is an illustration of an optical communications system that utilizes the programmable optical add/drop multiplexer of FIGS. 12a-12 c.

FIG. 14 is a diagram of a prior art switchable wavelength router.

DETAILED DESCRIPTION

The present invention provides an improved switchable interleaved channel separator. The following description is presented to enable one of ordinary skill in the art to make and use the invention and is provided in the context of a patent application and its requirements. Various modifications to the preferred embodiment will be readily apparent to those skilled in the art and the generic principles herein may be applied to other embodiments. Thus, the present invention is not intended to be limited to the embodiment shown but is to be accorded the widest scope consistent with the principles and features described herein.

To more particularly describe the features of the present invention, please refer to FIGS. 1a through 13 in conjunction with the discussion below.

FIG. 1a is a functional signal routing diagram of a switchable interleaved channel separator device in accordance with the present invention, as a 2×2 device. The switchable interleaved channel separator device 100 can be operated in either a first operational configuration, state “0” or in a second operational configuration, state “1”, as shown in the upper and lower diagrams of FIG. 1a, respectively. In the state “0”, odd-channel signals input to the switchable interleaved channel separator device 100 from Port A and from Port C are directed to Port B and to Port D, respectively, whereas even channel signals input to the switchable interleaved channel separator device 100 from Port A and from Port C are directed to Port D and to Port B, respectively. For instance, as shown in the upper diagram of FIG. 1a, in the state “0” the output at Port B consists of the odd channels (λ₁, λ₃, λ₅ . . . ) from the first composite optical signal λ₁-λ_(n) input at Port A plus the even channels (λ₂′, λ₄′, λ₆′ . . . ) from the second composite optical signal λ₁′-λ_(n)′ input at Port C. Further, in the state “0”, the output at Port D consists of the odd channels (λ₁′, λ₃′, λ₅′ . . . ) from the second composite optical signal plus the even channels (λ₂, λ₄, λ₆ . . . ) from the first composite optical signal. In the state “1”, the pathways of the odd channels and the even channels are reversed from those in the state “0” as shown in the lower diagram of FIG. 1a. In this way, the device 100 functions as a dense wavelength division multiplexer and de-multiplexer that discriminates amongst the pathways of odd and even channels and also functions as a 2×2 switch.

FIG. 1b is a functional signal routing diagram of the switchable interleaved channel separator device in accordance with the present invention, as a 1×2 device. The switchable interleaved channel separator device 150 (FIG. 1b) operates similarly to the device 100 (FIG. 1a) except that the device 150 only comprises one input port (Port A). In the state “0”, the switchable interleaved channel separator device 150 directs odd channels to Port B and even channels to Port D. In the state “1”, the odd channels are directed to Port D and the even channels are directed to Port B. In this way, the device 150 functions as a dense wavelength division multiplexer and de-multiplexer that discriminates amongst the pathways of odd and even channels and also functions as a 1×2 switch.

FIG. 2 is an illustration of a first preferred embodiment of a switchable interleaved channel separator device in accordance with the present invention. The switchable interleaved channel separator device 100. 1, shown in FIG. 2, is a modified version of an apparatus disclosed in U.S. Pat. No. 6,130,971, that is assigned to the assignee of the present applicant and which is incorporated herein by reference in its entirety. The 2×2 switchable interleaved channel separator device 100.1 (FIG. 2) comprises a first input optical fiber 210 and a second input optical fiber 240 for inputting optical signals and first 220 and second 230 output optical fibers for outputting optical signals. As an input composite optical signal leaves the first input optical fiber 210, it diverges. A first lens 250 collimates the input composite optical signal and directs it toward a polarization beam splitter 270 which decomposes the signal into two sub-signals having mutually orthogonal polarizations. The s-polarized portion of the input composite optical signal polarized parallel to a plane in the polarization beam splitter 270 is reflected towards a first adjustable non-linear interferometer 110 a. The p-polarized portion of the signal polarized perpendicularly to the plane in the polarization beam splitter 270 passes through towards a second adjustable non-linear interferometer 110 b.

Each of the adjustable non-linear interferometers 110 a and 110 b comprising the switchable interleaved channel separator device 100.1 is a modified instance of an invention disclosed in U.S. Pat. Nos. 6,169,604 and 6,310,690, both of which are assigned to the assignee of the present application and which are incorporated herein by reference in their entirety. Each of the adjustable non-linear interferometers 110 a and 110 b has the property such that, if the light beam reflected therefrom is an optical signal comprised of a plurality of wavelength division multiplexed channels and the light of each channel is linearly polarized, then the light of a first set of channels (for instance the “even” channels) is reflected with a 90° rotation of its polarization plane direction whilst the light of the remaining set of channels (for instance, the “odd” channels) is reflected with unchanged polarization. When light is input from the first input optical fiber 210 as shown in FIG. 2, the light comprising the set of channels whose polarization is rotated (the even channels, in this example) is directed to the second output optical fiber 230 and the light comprising the other set of channels (the odd channels, in this example) is directed to the first output optical fiber 220. When light is input from the second input optical fiber 240, the light comprising the set of channels whose polarization is rotated is directed to the first output optical fiber 220 and the light comprising the other set of channels is directed to the second output optical fiber 230.

It may be noted from the above description that, if fiber 210 is defined as Port A, fiber 220 is defined as Port B, fiber 230 is defined as Port D and fiber 240 is defined as Port C, then the device 100.1 functions as shown in the upper diagram of FIG. 1a. If the fiber 240 (Port C) is either absent or unutilized, then the device 100.1 functions as 1×2 device, as shown in the upper diagram of FIG. 1b. Furthermore, each of the adjustable non-linear interferometers 110 a-110 b of the switchable interleaved channel separator device 100.1 comprises two mutually exclusive states, whereby the set of channels (either even or odd) whose polarization plane is rotated may be selected. It is assumed that the two adjustable non-linear interferometers 110 a-110 b are always both in the same state. Thus, by toggling both adjustable non-linear interferometers 110 a-110 b from their first to second states and vice versa by mechanisms discussed further below, the output pathways of odd and even channels may be reversed. Thus, the device 100.1 can toggle between the two states shown in FIG. 1a.

FIG. 3 shows a side view of a second preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention. The switchable interleaved channel separator device 100.2, shown in FIG. 3, is a modified version of an apparatus disclosed in a co-pending U.S. patent application entitled “High-Isolation Dense Wavelength Division Multiplexer Utilizing Birefringent Plates and a Non-Linear Interferometer”, Ser. No. 09/404,005, filed Sep. 23, 1999. Applicant incorporates this patent application herein by reference in its entirety. In the device 100.2, reference numeral 515 is a four fiber ferrule and reference numerals 501, 502, 503 and 504 are four optical fibers, Fiber A, Fiber B, Fiber C and Fiber D, respectively, contained within and securely bonded to ferrule 515.

FIG. 4 shows an end view of the fiber configuration as viewed from the left side of the device of FIG. 3 utilized within the second preferred embodiment of the switchable interleaved channel separator device 100.2 in accordance with the present invention. Four collimator lenses, reference numerals 505, 506, 507 and 508, are incorporated into the end of ferrule 515 such that each collimator receives light from and directs light to exactly one of the fibers, specifically Fiber A 501, B 502, C 503 and D 504, respectively.

Disposed adjacent to the end of ferrule 515 is a first birefringent walk-off plate 509 that has the property of separating any signal light ray emanating from any of the fibers 501, 502, 503 or 504 into two physically separated linearly polarized sub-signal rays—one innermost and one outermost sub-signal ray. Because four fibers are contained within ferrule 515, eight separate sub-signals are so defined and are comprised of four outermost and four innermost sub-signals. The outermost and innermost sub-signals from both Fiber A 501 and Fiber B 502 comprise e-rays and o-rays, respectively, in their traverse through birefringent plate 509. Conversely, the outermost and innermost sub-signals from both Fiber C 503 and Fiber D 504 comprise o-rays and e-rays, respectively, in their traverse through birefringent plate 509. The polarization plane directions of these e-rays and o-rays are arbitrarily referred to as “horizontal” and “vertical,” respectively.

Disposed adjacent to the first birefringent plate 509 and on the side of plate 509 opposite to ferrule 515 are both a first half-wave plate 510 and a second half-wave plate 511. Half-wave plate 510 is aligned so as to intercept only the two outermost sub-signals arising from Fiber A 501 and Fiber B 502. Likewise, half-wave plate 511 is aligned so as to intercept only the two outermost sub-signals arising from Fiber C 503 and Fiber D 504. A second birefringent walk-off plate 512 is disposed adjacent to the two half-wave plates 510 and 511 on the side opposite to the first birefringent plate 509. The thickness of birefringent plate 512 is designed so as to give an offset of one of the rays propagating therethrough equivalent to the center-to-center distance between a pair of fibers. A lens or lens assembly 513 is disposed to the side of the second birefringent walk-off plate 512 opposite to the half wave plates 510 and 511. Finally, an adjustable non-linear interferometer 110, similar to each of the adjustable non-linear interferometers 110 a-110 b shown in FIG. 2, is disposed at the focal point of lens 513 opposite to the birefringent plate 512.

The operation of the switchable interleaved channel separator device 100.2 is illustrated in FIGS. 5a and 5 b. FIG. 5a is a sequence of cross sectional views 801-809 through the switchable interleaved channel separator device 100.2 (FIG. 3) illustrating the locations and polarization states of fiber images created by the light of signals and sub-signals of a first set of wavelength division multiplexed channels, whose polarization is not rotated by the adjustable non-linear interferometer 110. FIG. 5b is a sequence of cross sectional views 821-829 through the switchable interleaved channel separator device 100.2 (FIG. 3) illustrating locations and polarization states of fiber images created by the light of signals and sub-signals of a second set of wavelength division multiplexed channels, that are interleaved with the first set and whose polarization is rotated by 90° upon reflection from the adjustable non-linear interferometer 110. The identity of the channel set (e.g., either odd or even) whose light ray polarization is rotated depends upon the particular state of the adjustable non-linear interferometer 110. Thus, when the state of the adjustable non-linear interferometer 110 is in a first state “0”, FIG. 5a illustrates the pathways of odd channels and FIG. 5b illustrates the pathways of even channels. In a second state “1”, FIG. 5a illustrates the pathways of even channels and FIG. 5b illustrates the pathways of odd channels.

These cross-sections of FIGS. 5a-5 b are all drawn as viewed from the left side of the device of FIG. 3 and are taken at the labeled cross-sectional planes U-U′, V-V′, W-W′, X-X′, and Y-Y′ of FIG. 3. In FIGS. 5a and 5 b, circles drawn with solid lines are used to denote sub-signals comprised of vertically polarized light, circles drawn with dotted lines are used to denote sub-signals comprised of horizontally polarized light and adjacent solid and dotted circles are used to denote overlapping sub-signals of differing polarization or else signals of mixed or random polarization. The sizes of these circles have no physical significance. Reference numerals 810-811 represent fiber images of light originally input from Fiber A; reference numerals 812-813 represent fiber images of light originally input from Fiber B; reference numerals 814-815 represent fiber images of light originally input from Fiber C and reference numerals 816-817 represent fiber images of light originally input from Fiber D.

For a more-detailed description of the operation of the device 100.2 as illustrated in FIGS. 5a-5 b, please refer to the above-mentioned co-pending U.S. patent application Ser. No. 09/404,005. It is important to note that, when the adjustable non-linear interferometer 110 is in state “0”, odd-channel signal light input from Fiber A and Fiber C is output to Fiber B and Fiber D, respectively (FIG. 5a) whereas even-channel signal light input from Fiber A and Fiber C is output to Fiber D and Fiber B, respectively (FIG. 5b). Conversely, when the adjustable non-linear interferometer 110 is instate “1”, the output locations of odd and even channels are reversed. Therefore the device 100.2 operates according to the scheme illustrated in FIG. 1a. If the Fiber C is unused or absent, then the device 100.2 may be considered to operate as shown in FIG. 1b.

FIGS. 6a-6 c each illustrate a side view and a top view of a third preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention. The 1×2 switchable interleaved channel separator device 150.1, shown in FIGS. 6a-6 c, is a modified version of an apparatus disclosed in a co-pending U.S. Patent Application entitled “Multi-Functional. Optical Device Utilizing Multiple Polarization Beam Splitters and Non-Linear Interferometers,” Ser. No. 09/630,891, filed on Aug. 2, 2000. Applicant incorporates this patent application herein by reference in its entirety. The 1×2 switchable interleaved channel separator device 150.1 (FIGS. 6a-6 c) receives input from a first optical port 616 a and separates the channels therein into a first set of channels and a second set of channels that are interleaved with the first set of channels, wherein the first set is output to a first output optical port 616 b and the second set is output to a second output optical port 616 c, respectively. For reasons further detailed below, the optical ports 616 a-616 c are also referred to herein as polarizing ports.

As shown in FIG. 6a, the switchable interleaved channel separator device 150.1 further comprises a first 602 and a second 604 polarization beam splitter (PBS) between which are disposed a non-reciprocal optical rotation element 606 and a reciprocal optical rotation element 608. The first PBS 602 receives optical input from the input port 616 a which is disposed adjacent to a side of the PBS 602 opposite to the non-reciprocal rotator 606 and reciprocal rotator 608. An adjustable non-linear interferometer 110 is disposed adjacent to the second PBS 604 at a side opposite to the non-reciprocal rotator 606 and reciprocal rotator 608. The input port 616 a, first PBS 602, second PBS 604, non-reciprocal rotator 606, reciprocal rotator 608 and non-linear interferometer 110 are disposed along a line which defines a main axis or dimension of the device 150.1. Also shown in FIGS. 6a-6 c, as well as in several following figures of this document, are the polarization orientations of various signal light rays. These polarization orientations are indicated by double barbed arrows and/or crosses inscribed within circles. Unless otherwise indicated, double barbed arrows indicate light polarization along the indicated direction within the plane of the illustration, and crosses indicate light polarization normal to the plane of the page. Superimposed arrows and crosses either indicate non-polarized or randomly polarized light or superimposed rays which, in projection, have mutually perpendicular polarization plane orientations.

The switchable interleaved channel separator device 150.1 is further comprised of a first 612 and a second 614 optical reflector that are disposed adjacent to respective faces of the first PBS 602 and second PBS 604, neither of which faces intersect the main axis of the device 150.1. As shown in FIG. 6a, the optical reflectors 612-614 comprise right-angle prisms, but could also comprise mirrors. The two PBS's 602-604 each have the property of transmitting signal light comprising a first polarization (p-polarization) therethrough along the main axis whilst simultaneously deflecting signal light comprising a second polarization (s-polarization) to the adjacent optical reflector. Finally, the first output port 616b and the second output port 616c are disposed such that they receive light deflected by the first 612 and second 614 optical reflector, respectively.

FIG. 6d is a view of a polarizing input/output port assembly 616 utilized within the third preferred embodiment of the switchable interleaved channel separator device 150.1 in accordance with the present invention. The port 616 is herein termed a “polarizing port” because the port outputs light comprising only a single linear polarization orientation and can only receive light comprising the same linear polarization orientation.

The polarizing port 616 (FIG. 6d) comprises an optical fiber 680, an optical collimator 682, a birefringent walk-off plate 684 and a reciprocal optical rotator 686. The optical collimator 682 is optically coupled to the optical fiber 680 and either receives input from or directs output to the fiber 680. The birefringent walk-off plate 684 of the polarizing port 616 (FIG. 6d) is optically coupled to the collimator 682 at a side opposite to the fiber 680 and has the property of physically separating an unpolarized light beam received from collimator 682 into a deflected light beam 690 and an un-deflected light beam 688. The deflected light 690 comprises an e-ray having a first linear polarization orientation and the un-deflected light 688 comprises an o-ray having a second linear polarization orientation perpendicular to that of the e-ray. The reciprocal optical rotator 686, which is optically coupled to the birefringent walk-off plate 684 at a side opposite to the collimator 682, is disposed so at to intercept the path of only one of the two beams 688-690. The reciprocal optical rotator 686 rotates the polarization orientation of the intercepted beam by 90° so as to be parallel to that of the other beam. In the reverse light propagation direction, that is, when the polarizing port 616 is utilized as an output port, the optical rotator 686 rotates the polarization orientation of only one of two beams so that the beams subsequently comprise mutually orthogonal polarization orientations and such that these two beams are subsequently combined upon passage through the birefringent walk-off plate 684. The reciprocal optical rotator 686 may be disposed so as to intercept either the o-ray 688 or the e-ray 690.

The pathways and polarization orientations of forward propagating input signal rays within the switchable interleaved channel separator device 150.1 are shown in both top view (top diagram) and side view (lower diagram) in FIG. 6a. The return pathways (that is, the pathways after reflection from and interaction with the adjustable non-linear interferometer 110) of a first set of channels and of a second set of channels through the switchable interleaved channel separator device 150.1 are respectively shown in FIG. 6b and FIG. 6c.

Explicit details of the operation of the switchable interleaved channel separator device 150.1 are provided in the aforementioned co-pending U.S. Patent Application having Ser. No. 09/630,891. In summary, light of a composite optical signal, which is comprised of a plurality of wavelength division multiplexed channels λ₁-λ_(n), is input to the device 150.1 from input port 616 a with a single linear polarization orientation and propagates through the device 150.1 to the adjustable non-linear interferometer 110 (FIG. 6a). The adjustable non-linear interferometer 110 reflects the signal light such that the polarization plane of one set of channels is rotated by 90° whilst that of a second set of channels interleaved with the first set is not rotated. Further, the adjustable non-linear interferometer 110 can operate in either one of two states so as to select the particular set of channels whose light incurs polarization rotation. The light of the reflected channels then returns through the device 150.1 such that the light comprising the various channels is separated according to its polarization orientation.

The polarization orientations and pathways of the channels through the device 150.1 may be traced out using FIGS. 6a-6 c so as to verify that the device 150.1 operates as a 1×2 device according to the scheme shown in FIG. 1b. In these figures, it is assumed that the polarization plane of light comprising the even channels is rotated. It is to be noted that, during passage from right-to-left through the pair of elements 606-608, the polarization plane orientation of linearly polarized light is rotated by 90°, but, during passage from left-to-right through the pair of elements 606-608, the polarization plane orientation is not rotated.

FIGS. 7a-7 b are side views of a fourth preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention. In the switchable interleaved channel separator device 100.3 (FIGS. 7a-7 b), the three ports 616 a-616 c, first PBS 602, non-reciprocal optical rotator 606, reciprocal optical rotator 608, second PBS 604, adjustable non-linear interferometer 110 and optical reflector 612 are common to and disposed similarly to the respective similarly numbered components in the device 150.1 (FIGS. 6a-6 c). However, in the 2×2 switchable interleaved channel separator device 100.3 (FIGS. 7a-7 b), a third PBS 622 replaces the optical reflector 614, an additional input port 616 d is optically coupled to and disposed adjacent to a face of the third PBS 622 and an additional non-reciprocal optical rotator 618 and reciprocal optical rotator 620 are disposed between the third PBS 622 and the second PBS 604.

Details of the operation of the 2×2 switchable interleaved channel separator device 100.3 are provided in the aforementioned co-pending U.S. Patent Application having Ser. No. 09/630,891. The functionality of the 2×2 switchable interleaved channel separator device 100.3 (FIGS. 7a-7 b) with respect to a plurality of channels λ₁-λ_(n) input to the device 100.3 from input port 616 a is similar to that of the 1×2 switchable interleaved channel separator device 150.1 (FIGS. 6a-6 c). However, the 2×2 switchable interleaved channel separator device 100.3 comprises additional functionality beyond that of the 1×2 switchable interleaved channel separator device 150.1 with respect to the routing of a plurality of channels λ′₁-λ′_(n) that are input to the device 100.3 from the second input port 616 d. FIGS. 7a and 7 b respectively illustrate the pathways of the odd channels λ′₁, λ′₃, λ′₅, . . . and of the even channels λ′₂, λ′₄, λ′₆, . . . from the input port 616 d through the device 100.3 when the device 100.3 is in its state “0”. By following the pathways and polarization states of the signal light input from port 616 d as shown in FIGS. 7a and 7 b, it may be verified that, in the state “0”, the device 100.3 functions as shown in the upper diagram of FIG. 1a. The pathways of the odd channels and the even channels may be interchanged by toggling the adjustable non-linear interferometer 110 from one state to another as described in greater detail below.

FIGS. 8a-8 c are side views and top views of a fifth preferred embodiment of the switchable interleaved channel separator device in accordance with the present invention. The 1×2 switchable interleaved channel separator device 150.2, shown in FIGS. 8a-8 c, is a modified version of an apparatus disclosed in U.S. Pat. No. 6,396,629. Applicant incorporates this patent application herein by reference in its entirety. Like the device 150.1 previously described (FIGS. 6a-6 c), the 1×2 switchable interleaved channel separator device 150.2 (FIGS. 8a-8 c) receives input from a first optical port 616 a and separates the channels therein into a first set of channels and a second set of channels that are interleaved with the first set of channels, wherein the first set is output to a first output optical port 616 b and the second set is output to a second output optical port 616 c, respectively.

As shown in FIG. 8a, the switchable interleaved channel separator device 150.2 comprises a first 702 and a second 704 birefringent walk-off plate (or, simply termed, “birefringent plate”) between which are disposed a non-reciprocal optical rotator 706 and a reciprocal optical rotator 708. The first birefringent plate 702 receives optical input from the input port 616 a which is disposed adjacent to a side of the birefringent plate 702 opposite to the non-reciprocal rotator 706 and reciprocal rotator 708. An adjustable non-linear interferometer 110 is disposed adjacent to the second birefringent plate 704 at a side opposite to the non-reciprocal rotator 706 and reciprocal rotator 708. Finally, the first output port 616 b and the second output port 616 c are disposed to either side of the input port 616 a, wherein all three ports 616 a-161 c face the same side of the first birefringent plate 702. All three ports 616 a-616 c are polarizing ports of the type illustrated in FIG. 6d. The input port 616 a, first birefringent plate 702, second birefringent plate 704, non-reciprocal rotator 706, reciprocal rotator 708 and non-linear interferometer 110 are disposed along a line which defines a main axis or dimension of the switchable interleaved channel separator device 150.2.

The two birefringent plates 702-704 (FIG. 8a) each have the property of transmitting signal light comprising a first polarization (o-ray) therethrough substantially parallel to the main axis whilst simultaneously causing a deflection or offset of a signal light comprising a second polarization (e-ray). The path of the e-ray is deflected within either birefringent plate 702-704 but is substantially parallel to (thereby offset from) that of the o-ray immediately upon exiting the plate. The optical axes of the two birefringent plates 702-704 are disposed such that, for e-rays passing through both such birefringent plates 702-704 in a same direction, the offset of the e-ray immediately caused by passage through the second such birefringent plate 704 is equal and opposite to the offset of the e-ray immediately caused by the passage through the first birefringent plate 702. As oriented in FIGS. 8a-8 c, the e-rays and o-rays are polarized vertically and horizontally, respectively, during their traverses through the birefringent plates 702-704.

Explicit details of the operation of the switchable interleaved channel separator device 150.2 are provided in the aforementioned U.S. Pat. No. 6,396,629. In summary, light of a composite optical signal, which is comprised of a plurality of wavelength division multiplexed channels λ₁-λ_(n), is input to the device 150.2 from input port 616 a with a single linear polarization orientation and propagates through the device 150.2 to the adjustable non-linear interferometer 110 (FIG. 8a). The adjustable non-linear interferometer 110 reflects the signal light such that the polarization plane of one set of channels is rotated by 90° whilst that of a second set of channels interleaved with the first set is not rotated. Further, the adjustable non-linear interferometer 110 can operate in either one of two states so as to select the particular set of channels whose light incurs polarization rotation. The light of the reflected channels then returns through the device 150.2 such that the light comprising the various channels is separated according to its polarization orientation by the birefringent plates 702-704.

The polarization orientations and pathways of the channels through the device 150.2 may be traced out using FIGS. 8a-8 c. In these figures, it is assumed that the polarization plane of light comprising the even channels is rotated. It is to be noted that, during passage from right-to-left through the pair of elements 706-708, the polarization plane orientation of linearly polarized light is rotated by 90°, but, during passage from left-to-right through the pair of elements 706-708, the polarization plane orientation is not rotated.

FIGS. 9a-9 c illustrate three preferred embodiments of an adjustable non-linear interferometer 110 as utilized in the switchable interleaved channel separator device in accordance with the present invention. The non-linear interferometers 110.1 (FIG. 9a) 110.2 (FIG. 9b) and 110.3 (FIG. 9c) are modifications of an invention disclosed in the co-pending U.S. Pat. Nos. 6,169,604 and 6,310,690.

The adjustable non-linear interferometer 110.1 (FIG. 9a) comprises two glass plates 580A-580B optically coupled to one another, wherein the first glass plate 580A comprises a wedge shape. The inside face of the second glass plate 580B is coated with a layer of reflective coating 520 with a reflectivity preferably of 100%. The inside face of the first glass plate 580A is substantially parallel to the inside face of plate 580B and is coated with a layer of a partially reflective coating 540 with a reflectivity less than 100%. The two glass plates are separated by spacers 512, such that an interferometric cavity 510 is created between the partially reflective coating 540 and the 100% reflective coating 520. The spacers 512 preferably comprise a zero-thermal-expansion or low-thermal-expansion material. The adjustable non-linear interferometer 110.1 further comprises a first birefringent waveplate 582 disposed external to the cavity 510 and optically coupled to the glass plate 580A and a second birefringent waveplate 595 disposed within the cavity 510 and optically coupled to the glass plates 580A-580B. An input linearly polarized light 504 comprised of multiple channels is reflected as light 505, wherein the polarization of a first set of channels is rotated and the polarization of a second set of channels interleaved with the first set of channels is not rotated.

As described in more detail in the aforementioned co-pending U.S. Pat. No. 6,310,690, the reflectivity, r₁, of the partially reflective coating 540 and the optical retardance (or retardation), L₁, of the external waveplate 582 and the optical retardance, L₂, of the internal waveplate 595, may be independently varied so as to vary the optical properties of the non-linear interferometer. Specifically, when L₁=λ/8, L₂=λ/4 and r₁=18.5%, then the channels of the set comprising the rotated polarization light and channels of the set comprising the non-rotated polarization light have similar spectral bandwidths. In another example, when L₁=3λ/16, L₂=λ/8 and r₁=32.5%, then the channels of the set comprising the rotated polarization light and the channels of the set comprising the non-rotated polarization light have spectral bandwidths that are in a ratio of 3:1 (or 1:3). In yet another example, when L₁=7λ/32, L₂=λ/16 and r₁=56.3%, then the channels of the set comprising the rotated polarization light and the channels of the set comprising the non-rotated polarization light have spectral bandwidths that are in a ratio of 7:1 (or 1:7). In each case the first and second sets of channels are interleaved with one another.

Each of the adjustable non-linear interferometers 110.1-110.3 (FIGS. 9a-9 c) may be changed from a first operational state to a second operational state by adjusting the optical path length L₀ of the cavity 510. In a first operational state, upon reflection from the adjustable non-linear interferometer 110.1-110.3, the polarization of the light of a first set of channels is rotated by 90° whilst the polarization of the light of a second set of channels is not rotated. In a second operational state, the polarization of the light of the second set of channels is rotated by 90° whilst the polarization of the light of the first set of channels is not rotated.

The principle that permits the change of operational states of the adjustable non-linear interferometers 110.1-110.3 is illustrated in FIG. 9d, which presents two schematic graphs of the spectrum 320 of passbands of the polarization-rotated light and the spectrum 322 of passbands of non-polarization-rotated light. The upper and lower graphs of FIG. 9d represent the spectra of passbands reflected from an adjustable non-linear interferometer in a first operational state “0” and in a second operational state “1”, respectively. The locations of“odd” channels 324 and of“even” channels 326 are also shown in the graphs of FIG. 9d. As is well known, the free spectral range (in terms of frequency) of a reflective interferometer of the type shown in FIGS. 9a-9 c is inversely proportional to the optical path length L₀, of the cavity 510. Thus, when this optical path length is increased or decreased, the spectra 320-322 of passbands effectively “shift” to either the left or the right accordingly. A very slight change in the passband widths also accompanies this shift, but this effect is negligible in regards to the operation of any of the adjustable non-linear interferometers 110.1-110.3. The effect of the shift of the spectra of passbands is to cause the spectrum of polarization rotated light (non-polarization-rotated light) to either coincide with the locations of the even channels or the odd channels (odd channels or the even channels), depending upon the selected operational state, as may be seen be comparing the two graphs of FIG. 9d.

Within the adjustable non-linear interferometer 110.1 (FIG. 9a), the internal birefringent waveplate 595 is disposed within the cavity 510 at a certain “tilt” angle α with respect to the parallel reflective surfaces 520 and 540. The optical path length L₀ between the parallel reflective surfaces 520 and 540 depends, in part, on the optical path length L₅₉₅ through the optical length adjustment element. This quantity L₅₉₅ is, in turn, related to the physical path length of signals 504-505 through the element 595 as well as the principal refractive indices of element 595. Since, this physical path length depends upon the tilt angle a of element 595, then it follows that the quantity L₅₉₅ and the quantity L₀ depend upon the angle α. Thus, by adjusting the angle α, it is possible to tune the phase of the channels comprising the reflected light 505. The angle a may be adjusted by means of a mechanical tilt adjustment mechanism (not shown) so that the phase of the reflected channels may be varied during operation of the switchable interleaved channel separator device within which the adjustable non-linear interferometer is utilized. These phase changes cause the shifts of the passband spectra 320-322 (FIG. 9d).

The adjustable non-linear interferometer 110.2 shown in FIG. 9b comprises all the elements (“cavity elements”) of the interferometer 110.1 (FIG. 9a) in addition to a piezoelectric element 522 attached to the second glass plate 580B. Instead of being disposed on the second glass plate 580B, the 100% reflective coating comprising the adjustable non-linear interferometer 110.2 is disposed upon the piezoelectric element 522 facing into the cavity 510 (FIG. 9b). By controlling a voltage applied across the piezoelectric element 522, the variable thickness t of the piezoelectric element 522 may be very accurately controlled. This property of piezoelectric materials is well known. In this fashion, the optical path length L₀ between the parallel reflective surfaces 520 and 540 may be controlled. Thus, by adjusting the thickness t, it is possible to control the phase of the reflected channels 505. The internal waveplate 595 is disposed in a fixed position—that is, without a tilt adjustment—within the adjustable non-linear interferometer 110.2.

The adjustable non-linear interferometer 110.3 shown in FIG. 9c comprises all the elements of the interferometer 110.1 (FIG. 9a). However, in the adjustable non-linear interferometer 110.3, the “cavity elements” are disposed within a hermetically sealed enclosure 584. Preferably, the external waveplate 582 is disposed outside of the enclosure 584, but could also be within the enclosure. A window 588 comprising non-parallel surfaces is bonded to the enclosure and permits the previously described optical couplings to be maintained. In operation, a positive air pressure is maintained within the enclosure 584. The exact pressure within the enclosure 584 may be varied by forcing gas into or extracting gas from the enclosure via the inlet tube 586. These controlled variations in gas pressure within the enclosure cause slight expansions or contractions of the interferometer elements within the enclosure such that the optical path length between the two reflective surfaces 520 and 540 may be varied in a controlled fashion. The variation of optical path length is sufficient to vary the phase of the reflected channels 505. The internal waveplate 595 is disposed in a fixed position—that is, without a tilt adjustment—within the adjustable non-linear interferometer 110.3.

FIG. 10 is an illustration of a first preferred embodiment of an optical communications system that utilizes the switchable interleaved channel separator device in accordance with the present invention. This dense wavelength division multiplexing (DWDM) system 900 comprises a plurality of switchable interleaved channel separator devices (150 a, 150 b, 150 c . . . ), each of which functions as a 1×2 switch as illustrated in FIG. 1b. The DWDM system 900 has a programmable parallel cascade router configuration, since each of the switchable interleaved channel separator devices (150 a, 150 b, 150 c, . . . ) may be programmed to route particular channels to particular paths. This programmable parallel cascade router configuration is disclosed in a co-pending U.S. Pat. No. 6,263,126 assigned to the assignee of the present application. Applicant incorporates this patent application herein by reference in its entirety.

The DWDM 900 comprises an optical input 102, a plurality of switchable interleaved channel separator devices 150 a, 150 b, 150 c, . . . optically coupled in a parallel cascade configuration by a plurality of optical couplings 104 a, 104 b, 104 c, . . . and a plurality of optical outputs 106 a, 106 b, 106 c, . . . , wherein the input 102 carries a wavelength division multiplexed composite optical signal and each output carries an individual signal or channel. Generally the optical input, the optical outputs and the optical couplings will all comprise optical fibers, but may comprise, in whole or in part, any form of optical coupling devices, such as lenses, mirrors, prisms, windows, etc. For clarity, it is assumed that the input composite optical signal to the DWDM 900 comprises the eight channels λ₁-λ₈ and, thus, the eight optical outputs 106 a-106 h, the seven switchable interleaved channel separator devices 150 a-150 g and the six optical couplings 104 a-104 f are utilized. However, the input composite optical signal to the DWDM 900 may comprise any number of channels and the number of switchable interleaved channel separator devices, optical couplings and optical outputs may vary accordingly.

The switchable interleaved channel separator devices 150 a-150 g of the DWDM 900 are arranged in a parallel cascade configuration such that: (1) the two outputs of the device 150 a are optically coupled to the device 150 b and the device 150 c via the optical couplings 104 a and 104 b, respectively; (2) the two outputs of the device 150 b are optically coupled to the device 150 d and the device 150 e via the optical couplings 104 c and 104 d, respectively; (3) the two outputs of the device 150 c are optically coupled to the device 150 f and the device 150 g via the optical couplings 104 e and 104 f, respectively and (4) each of the devices 150 d-150 g is optically coupled to a pair of the optical outputs 106 a-106 h. The spacing between passbands of the devices 150 b-150 c is twice that of the passband spacing of device 150 a. The passband spacing of the devices 150 d-150 g is twice that of the passband spacings of devices 150 b-150 c.

In the example illustrated in FIG. 10, the first switchable interleaved channel separator device 150 a is in state “1” (see FIG. 1b) and thus routes the odd channels (λ₁, λ₃, λ₅, λ₇) to device 150 c and the even channels (λ₂, λ₄, λ₆, λ₈) channels to the device 150 b. Device 150 b, also in state “1”, routes λ₄ and λ₈ to device 150 d, and routes λ₂ and λ₆ to device 150 e. However, the device 150 c is in state “0” (in this example) and thus routes channels λ₃ and λ₇ to device 150 g, and routes λ₁ and λ₅ to device 150 f. Similarly, the devices 150 e and 150 f are in the state “1” whereas the devices 150 d and 150 g are in the state “0”, resulting in the particular set of outputs to ports 106 a-106 h as shown in FIG. 10. In the example shown in FIG. 10, there are seven different independent 1×2 devices 150 a-150 g which may be programmed independently of one another. There are therefore 2⁷(=128) different possible permutations of the output signals among the outputs 106 a-106 h.

FIG. 11 illustrates a second preferred embodiment of an optical communications system that utilizes the switchable interleaved channel separator device in accordance with the present invention. The system 1000 (FIG. 11) comprises a plurality of switchable interleaved channel separator devices (100 a, 100 b, 100 c, . . . ) each of which functions as a 2×2 switch as illustrated in FIG. 1a. In the example illustrated in FIG. 11, a first wavelength division multiplexed composite optical signal comprising the channels λ₁-λ₈ is input to the set of channel separators 920 a-920 c and a second wavelength division multiplexed composite optical signal comprising the channels λ₁′-λ₈′ is input to the set of channel separators 920 d-920 f. The set of channel separators 920 a-920 c and the set of channel separators 920 d-920 f are each configured in a parallel cascade arrangement as disclosed in the aforementioned co-pending U.S. Patent Application having Ser. No. 09/130,386. Therefore, the two outputs of the channel separator 920 b comprise the set of channels λ₄, λ₈) and the set of channels (λ₂, λ₆), respectively. The two outputs of the channel separator 920 c comprise the set of channels λ₃, λ₇) and the set of channels (λ₁, λ₅), respectively. Likewise, the two outputs of the channel separator 920 e comprise the set of channels λ₄′, λ₈′) and the set of channels (λ₂′, λ₆′), respectively and the two outputs of the channel separator 920 f comprise the set of channels (λ₃′, λ₇′), and the set of channels (λ₁′, λ₅′), respectively.

Within the system 1000 (FIG. 11), the “4” and “8” channels, that is, the set of channels (λ₄, λ₈) and the set of channels (λ₄′, λ₈′), are input to the 2×2 switchable interleaved channel separator device 100 a. Likewise, the “2” and “6” channels from each original composite optical signal are input to the 2×2 switchable interleaved channel separator device 100 b, the “3” and “7” channels are input to the 2×2 switchable interleaved channel separator device 100 c and the “1” and “5” channels are input to the 2×2 switchable interleaved channel separator device 100 d. Each of the 2×2 switchable interleaved channel separator devices 100 a-100 d may be in one of two different switch states, “0” or “1”. One output of each of the devices 100 a-100 d is directed to the set of channel separators 920 g-920 i and the other output of each of the devices 100 a-100 d is directed to the set of channel separators 920 j-920 l. The switch state of each of the devices 100 a-100 d determines the particular routings of the wavelengths to the outputs, as described previously with reference to FIG. 1a. The set of channel separators 920 g-920 i and the set of channel separators 920 j-920 l are each configured in a parallel cascade arrangement so as to re-combine the various channels. For the particular set of switch states illustrated in FIG. 11, the channels λ₁′, λ₂, λ₃, λ₄′, λ₅, λ₆′, λ₇′ and λ₈ are routed to as to be output from system 1000 via the channel separator 920 i and the channels λ₁, λ₂′, λ₃′, λ₄, λ₅′, λ₆, λ₇ and λ₈′ are routed so as to be output via channel separator 920 l. For the example shown in FIG. 11, there are a total of sixteen different unique routing configurations of the system 1000.

FIGS. 12a-12 c illustrate a programmable optical add/drop multiplexer (OADM) that utilizes the switchable interleaved channel separator device in accordance with the present invention. The OADM 1100 (FIGS. 12a-12 c) comprises a plurality of switchable interleaved channel separator devices (100 a, 100 b, 100 c . . . ) each of which functions as a 2×2 switch as illustrated in FIG. 1a. FIGS. 12a-12 b illustrate two different operational examples or states of the OADM 1100 wherein the OADM 1100 comprises three such switchable interleaved channel separator devices 100 a-100 c. FIG. 12c illustrates an example wherein the apparatus 1100 comprises two switchable interleaved channel separator devices 100 a-100 b. In each of the three operational examples shown in FIGS. 12a-12 c, it is assumed that a composite optical signal comprising channels λ₁-λ₈ is input into the OADM 1100 via an optical input 902 and that the passband spacing of each switchable interleaved channel separator device is twice that of the immediately preceding device and one half of that of the immediately following device.

Referring now to the example shown in FIG. 12a, the first switchable interleaved channel separator device 100 a separates the input composite optical signal into its odd (λ₁, λ₃, λ₅, λ₇) and even (λ₂, λ₄, λ₆, λ₈) channels. Since the device 100 a is in a state “1” (in this example), the odd channels are directed, via optical coupling 908, to the device 100 b, which further separates them into two sets of channels, (λ₁, λ₅) and (λ₃, λ₇). Since the device 100 b is in a state “0”, the (λ₃, λ₈) set of channels is directed, via the optical coupling 912, to the device 100 c which separates them into the separate channels λ₃ and λ₇. Since the device 100 c is in a state “1”, the channel λ₃ is then dropped to the drop line 916. Since the channel λ₃ is dropped, a new signal λ₃′ comprising the same wavelength as λ₃ may be simultaneously added as an input into the device 100 c from the add line 904. Since the device 100 c acts as a 2×2 switch and is in the state “1” as described previously, channel λ₃′ is then added to λ₇ by the device 100 c. This signal is looped back, via optical coupling 914, as an input to the device 100 b, which, since it is in state “0”, adds λ₇ and λ₃′ to λ₁ and λ₅. This combined signal is looped back, via optical coupling 910, as an input to the device 100 a, which, since it is in state “1”, adds channels λ₁, λ₅, λ₇, λ₃′ to channels λ₂, λ₄, λ₆, λ₈, resulting in one optical signal containing channels λ₁, λ₂, λ₃′, λ₄, λ₅, λ₆, λ₇, and λ₈. This new signal is then output from the DWDM 1100 along the express line 906. Thus, in this manner, channel λ₃ is dropped while channel λ₃′ is added.

FIG. 12b illustrates an additional example of a different operational state of the OADM 1100. Since, in the examples of FIGS. 12a-12 b, the OADM 1100 comprises three switchable interleaved channel separator devices 100 a-100 c, wherein each such device may be in one of two states, there are a total of 2³(=8) possible operational states for the OADM 1100, each of which corresponds to adding and dropping of a different one of the eight possible wavelengths. It is to be noted, however, that the OADM 1100 may comprise any number of switchable interleaved channel separator devices and that the composite optical signal may comprise any number of channels. FIG. 12b illustrates the situation in which the three switchable interleaved channel separator devices 100 a-100 c are in the states “1”, “0” and “0”, respectively, and thus channel λ₇ is dropped and channel λ₇′ is added. More generally, for 2^(n) channels and m (m≦n) stages, 2^(n−m) channels may be dropped. In the further example shown in FIG. 12c, the OADM 1100 comprises two stages (that is, m=2) and thus two channels may be simultaneously dropped and added.

FIG. 13 illustrates an optical communications system that utilizes the optical add/drop multiplexer of FIG. 1a-12 c. The system 1200 drops a different channel from a composite optical signal at each one of a series of nodes within an optical network. The nodes are represented by the reference numerals 1201 a, 1201 b, 1201 c, . . . in the programmable optical communications system 1200 shown in FIG. 13. Each node comprises one of a plurality of programmable OADM's 1100 a, 1100 b, 1100 c, . . . , one of a plurality of optical drop lines 1203 a, 1203 b, 1203 c, . . . , one of a plurality of optical taps 1204 a, 1204 b, 1204 c, . . . , one of a plurality of optical tap lines 1205 a, 1205 b, 1205 c, . . . , one of a plurality of controllers 1202 a, 1202 b, 1202 c, . . . , and one of a plurality of electronic control lines 1206 a, 1206 b, 1206 c, . . . . Within each node 1201 a, 1201 b, 1201 c, . . . comprising the system 1200, an optical tap line 1205 a, 1205 b, 1205 c, . . . is optically coupled between an optical tap 1204 a, 1204 b, 1204 c, . . . and a controller 1202 a, 1202 b, 1202 c, . . . ; a programmable OADM 1100 a, 1100 b, 1100 c, . . . is optically coupled to an optical drop line 1203 a, 1203 b, 1203 c, . . . and to an optical tap and to at least one other node 1201 a, 1201 b, 1201 c, . . . , and an electronic control line 1206 a, 1206 b, 1206 c, . . . is electronically coupled between a controller 1202 a, 1202 b, 1202 c, . . . and an OADM 1100 a, 1110 b, 1100 c, . . . , Preferably, each one of the programmable OADM's 1100 a, 1100 b, 1100 c, . . . comprises the structure shown in FIGS. 12a-12 b.

The first node 1201 a in the programmable system 1200 receives a composite optical signal comprising the channels λ₁-λ_(n) as well as an optical service channel λ^(s) from the optical network. The optical service channel λ^(s) comprises a wavelength that is different from those of any of the regular channels and carries information related to the routing of various channels within the programmable system 1200. This information is utilized and decoded by each of the controllers 1202 a, 1202 b, 1202 c, . . . so that the appropriate channel is dropped to the drop line 1203 a, 1203 b, 1203 c, . . . at each node 1201 a, 1201 b, 1201 c, . . . Within each node 1201 a, 1201 b, 1201 c, . . . , the controller 1202 a, 1202 b, 1202 c, . . . sends appropriate control signals to the programmable OADM 1100 a, 1100 b, 1100 c, . . . through the electronic control line 1206 a, 1206 b, 1206 c, . . . The control signals cause the set of switchable interleaved channel separator devices comprising the programmable OADM 1100 a, 1100 b, 1100 c, . . . to assume the appropriate switch states such that the correct wavelength channel is dropped at each node. In this system 1200, no signals are added at the nodes 1201 a, 1201 b, 1201 c, . . . . Therefore, upon exiting from each node, the composite optical signal that propagates to the subsequent node comprises one less channel than that entering the node.

An improved switchable interleaved channel separator device, and methods and systems utilizing the device in fiber optic communications networks, have been disclosed. The switchable interleaved channel separator device utilizes an adjustable reflective non-linear interferometer, which performs both switching and wavelength polarization sorting functions, so that overall complexity of the device is reduced. Further, because the adjustable non-linear interferometer is a reflection element, signal light paths are folded back upon one another so as to realize an overall reduction in the device's size, as well as the capability of performing optical couplings predominantly or wholly at a single side or at adjacent sides of the device.

Although the present invention has been described in accordance with the embodiments shown, one of ordinary skill in the art will readily recognize that there could be variations to the embodiments and those variations would be within the spirit and scope of the present invention. Accordingly, many modifications may be made by one of ordinary skill in the art without departing from the spirit and scope of the appended claims. 

What is claimed is:
 1. A switchable interleaved channel separator device, comprising: at least one input port for inputting at least one optical signal in a forward direction; a separating means optically coupled to the at least one input port for separating the at least one optical signal traversing through the separating means in a direction into a first set of channels and a second set of channels interleaved with the first set of channels; at least one adjustable non-linear interferometer (ANLI) optically coupled to the separating means, wherein the at least one ANLI in a first state rotates a polarization of the first set of channels, wherein the at least one ANLI in a second state rotates a polarization of the second set of channels, and wherein the at least ANLI reflects the first and second sets of channels to the separating means in the return direction; a first output port optically coupled to the separating means for outputting the first set of channels when the at least one ANLI is in the first state and the second set of channels when the at least one ANLI is in the second state; and a second output port optically coupled to the separating means for outputting the second set of channels when the at least one ANLI is in first state and the first set of channels when the at least one ANLI is in the second state, wherein the separating means comprises: a first birefringent plate optically coupled to the at least one input port, a set of optical rotators optically coupled to the first birefringent plate, the set of optical rotators comprising a NRR and a RR, and a second birefringent plate optically coupled to the set of optical rotators at a side opposite to the first birefringent plate, wherein the at least one ANLI is optically coupled to the second birefringent plate at a side opposite to the set of optical rotators.
 2. The device of claim 1, wherein the at least one input an optical collimator; a birefringent walk-off plate optically coupled to the optical collimater; and an input reciprocal optical rotator intercepting a portion of a light from the birefringent walk-off plate.
 3. A switchable interleaved channel separator device, comprising: at least one input port for inputting at least one optical signal in a forward direction; a separating means optically coupled to the at least one input port for separating the at least one optical signal traversing through the separating means in a return direction into a first set of channels and a second set of channels interleaved with the first set of channels, wherein the separating means comprises: a first birefringent plate optically coupled to the at least one input port, a set of optical rotators optically coupled to the first birefringent plate, the set of optical rotators comprising a NRR and a RR, and a second birefringent plate optically coupled to the set of optical rotators at a side opposite to the first birefringent plate, wherein at least one ANLI is optically coupled to the second birefringent plate at a side opposite to the set of optical rotators; the at least one ANLI optically coupled to the separating means, wherein the at least one ANLI in a first state rotates a polarization of the first set of channels, wherein the at least one ANLI in a second state rotates a polarization of the second set of channels, and wherein the at least one ANLI reflects the first and second set of channels to the separating means in the return direction: a first output port optically coupled to the separating means for outputting the first set of channels when the at least one ANLI is in the first state and the second set of channels when the at least one ANLI is in the second state; and a second output port optically coupled to the separating means for outputting the second set of channels when the at least one ANLI is in the first state and the first set of channels when the at least one ANLI is in the second state.
 4. The device of claim 3, wherein the at least one input port comprises: an optical collimator; a birefringent walk-off plate optically coupled to the optical collimator; and an input reciprocal optical rotator intercepting a portion of a light from the birefringent walk-off plate.
 5. A system, comprising: an optical input; and a plurality of switchable interleaved channel separator devices optically coupled to the optical input, wherein the plurality of switchable interleaved channel separators are optically coupled in a parallel cascade configuration, wherein each switchable interleaved channel separator device comprises: an input port for inputting an optical signal in a forward direction, a separating means optically coupled to the input port for separating the optical signal traversing through the separating means in a return direction into a first set of channels and a second set of channels interleaved with the first set of channels, at least one ANLI optically coupled to the separating means, wherein the at least one ANLI in a first state rotates a polarization of the first set of channels, wherein the at least one ANLI in a second state rotates a polarization of the second set of channels, and wherein the at least one ANLI reflects the first and second set of channels to the separating means in the return direction, a first output port optically coupled to the separating means for outputting the first set of channels when the at least one ANLI is in the first state and the second set of channels when the at least one ANLI is in the second state, and a second output port optically coupled to the separating means for outputting the second set of channels when the at least one ANLI is in the first state and the first set of channels when the at least one ANLI is in the second state, wherein the separating means comprises: a first birefringent plate optically coupled to the at least one input port, a set of optical rotators optically coupled to the first birefringent plate, the set of optical rotators comprising a NRR and a RR, and a second birefringent plate optically coupled to the set of optical rotators at a side opposite to the first birefringent plate, wherein the at least one ANLI is optically coupled to the second birefringent plate at a side opposite in the set of optical rotators.
 6. The system of claim 5, wherein the at least one input port comprises: an optical collimator; a birefringent walk-off plate optically coupled to the optical collimator; and an input reciprocal optical rotator intercepting a portion of a light from the birefringent walk-off plate. 